ARMOR-PIERCING FORGED STEEL SHELL.

6-inch, 3 calibers long, weight 100 lb, charge 11/2 lb.

8 " " " 250 " 3 "

10 " " " 500 " 51/2 "

12 " " " 850 " 11 "

The chief efficiency of small quantities of high explosives having

reduced itself to the case of armor-piercing projectiles, it next

became evident that there was an entirely new field for high

explosives into which powder had entered but little, and this was the

introduction of huge torpedo shells, which did nor rely for their

efficiency upon the dispersion of the pieces of the shell, but upon

the devastating force of the bursting charge itself upon everything

within the radius of its explosive effect. It is in this field that we

may look for the most remarkable results, and it is here that the

absolute power of the explosive thrown is of the utmost importance,

provided that it can be safely used. Attention was at once turned in

Europe to the manufacture of large projectiles with great capacity for

bursting charges, and it has resulted in the production of a class of

shells 41/2 to 6 calibers long, with walls only 0.4 of an inch thick.

(If they are made thinner, they will swell and jam in the gun when

fired.)

These shells are used in long guns up to 6 and 81/2 inches caliber, and

in mortars up to 11.2 inches. They are made from disks of steel, 3 to

4 feet in diameter and 1 inch thick, and are forced into shape by

hydraulic presses. The base is usually screwed in, but some of the

German shell are made in two halves which screw together. The Italians

were the first in this new field of investigation, but the Germans

soon followed, and after trying various materials were at length

reasonably successful with gun-cotton soaked in paraffin. Their 8.4

inch mortar shells of 5 calibers contain 42 pounds; those of 6

calibers contain 57 pounds; and the 11.2 inch mortar shells of 5

calibers contain 110 pounds.

The projectile velocity used with the mortars is about 800 f.s. The

effect of these shells against ordinary masonry and earth

fortifications is very great. The charge of forty-two pounds has

broken through a masonry vault of three feet four inches thick,

covered with two feet eight inches of cement and with three to five

feet of earth over all. The shell containing fifty-seven pounds, at a

range of two and one-half miles, broke through a similar vault covered

with ten feet of earth; but with seventeen feet of earth the vault

resisted. In 1883, experiments at Kummersdorf showed that a shell

containing the fifty-seven pound charge would excavate in sand a

crater sixteen feet in diameter and eight feet deep, with a capacity

of twenty-two cubic yards. The Italians have had similar experiences;

but it is notable that in both Germany and Italy several guns and

mortars have burst. The velocity in the guns is not believed to exceed

1,200 to 1,300 f.s., and it is not thought that the quantity of

gun-cotton is as great in the gun shells as in the mortars. I have

lately been informed on good authority that the use of gun-cotton

shells has been abandoned in the German navy as too dangerous.

The French, in their investigations in this field, found gun-cotton

too inconvenient, and decided upon melenite. This substance has

probably attracted more attention in the military world than all

others combined, on account of the fabulous qualities that have been

ascribed to it. Its composition was for a long time entirely a secret;

but it is now thought to consist principally of picric acid, which is

formed by the action of nitric acid upon phenol or phenyillic alcohol,

a constituent of coal tar. The actual nature of melenite is not

positively known, as the French government, after buying it from the

inventor, Turpin, are said to have added other articles and improved

it. This is probable, since French experiments in firing against a

partially armored vessel, the Bellequense, developed an enormous

destructive effect, while the English, who afterward bought it,

conducted similar experiments against the Resistance, and obtained no

better results than with powder. The proof that the Bellequense

experiments were deemed of great value by the French lies in the fact

that they immediately laid down a frigate--Dupuy de Lome--in which

four-inch armor is used, not only on the side, but about the gun

stations, to protect the men; this thickness having been found

sufficient to keep out melenite shell. In most armorclads, the armor

is very heavy about the vitals, but the guns are frequently much

exposed.

The best authenticated composition for melenite consists of picric

acid, gun cotton and gum arabic, and lately it is stated that the

French have added cresilite to it. Cresilite is another product of

coal tar. Melenite is normally only three times as strong as

gunpowder; but it is said to owe its destructive qualities in shells

to the powerful character of the exploder which ignites it. It has

been known for some years that all explosives (including gunpowder)

are capable of two orders of explosion according as they are merely

ignited or excited by a weak fuse or as they are powerfully shocked by

a more vigorous excitant. Fulminate of mercury has been found most

serviceable for the latter purpose. With melenite the French have

reproduced all the results that the Germans have effected with

gun-cotton and have found that a shell containing 119 pounds of it

will penetrate nearly ten feet of solid cement, but will not penetrate

armored turrets six to eight inches thick. The French claim that

melenite has an advantage over gun-cotton in not being so dangerous to

handle and being insensible to shock or friction, and they have

obtained a velocity of 1,300 f.s. with the 88 inch mortar and claim to

have obtained 2,000 f.s. in long guns up to 62 inch caliber. However

this may be, they are known to have had severe accidents at the

manufactory at Belfort and at least one 56 inch gun was burst at the

Bellequense experiments in firing a sixty-six pound shell containing

twenty-eight pounds of melenite. The French are said to have large

quantities of melenite shells in store, but they are not issued to

service.

Probably one reason why we have so many conflicting yet positive

accounts of great successes in Europe with torpedo shells is because

each nation wishes its neighbors to think that it is prepared for all

eventualities, and they are obliged to keep on hand large quantities

of some explosive, whether they have confidence in it or not.

Fortunately we are not so situated, but singularly enough what we have

done in the field of high explosive projection has been accomplished

by private enterprise, and we have attacked the problem at exactly the

opposite point from which European nations have undertaken it. While

they have assumed that the powder gun with its powerful and relatively

irregular pressures was a necessity and have endeavored to modify the

explosive to suit it, we have taken the explosive as we have found it,

and have adapted the gun to the explosive. At present the prominent

weapon in this new field is the pneumatic gun, but it is obvious that

steam, carbonic acid gas, ammonia or any other moderate and

regulatable pressure can be used as well as compressed air; it is

merely a question of mechanical convenience.

In throwing small quantities of certain high explosives, powder guns

can be used satisfactorily, but when large quantities are required,

the mechanical system of guns possess numerous advantages. All the

high explosives are subject to premature detonation by shock; each of

them is supposed to have its own peculiar shock to which it is

sensitive; but what this shock may be is at present unknown. We do

know, however, that premature explosions in guns are more liable to

occur when the charge in the shell is large than when it is small.

This is due to the fact that when the gun is fired, the inertia of the

charge in the shell is overcome by a pressure proportional to the mass

and acceleration, which pressure is communicated to the shell charge

by the rear surface of the cavity, and the pressure per unit of mass

will vary inversely as this surface. If, then, the quantity of

explosive in the shell forms a large proportion of the total weight of

the shell, we approach in powder guns a condition of shock to it which

is always dangerous and frequently fatal. The pressure behind the

projectile varies from twelve to fifteen tons per square inch, but it

is liable to rise to seventeen and eighteen tons, and in the present

state of the manufacture of gunpowder we cannot in ordinary guns

regulate it nearer than that. It is not a matter of so much importance

so far as the guns are concerned, when using ordinary projectiles, as

the gun will endure a pressure of from twenty-five to thirty tons per

square inch; but with high explosives in the shell it is a vitally

serious matter. From all I can learn regarding European practice, it

appears that not only are the explosives made sluggish, but the

quantity seldom exceeds thirty per cent. of the weight of the shell,

and the velocities, notwithstanding, are kept very low. In the

pneumatic gun the velocity is low also, but so is the pressure in the

gun. The pressure in the firing reservoir is kept at the relatively

low figure of 1,000 pounds per square inch or less, and the air is

admitted to the chamber of the gun by a balance valve which cuts off

just the quantity of air (within a very few pounds) that is required

to make the shot. The gun is long, and advantage is taken of the

expansion of the air. In no case can the pressure rise in the gun

beyond that in the reservoir.

Up to the present time there have been no accidents in using the most

powerful explosives in their natural state, and in quantities over

fifty per cent. of the weight of the projectile. I have seen

projectiles weighing 950 pounds, and containing 500 pounds of

explosives (300 pounds of the blasting gelatine and 200 pounds of No.

1 dynamite) thrown nearly a mile and exploded after disappearing under

water. According to Gen. Abbot's formula such a projectile would have

sunk any armorclad floating within forty-seven feet of where it

struck. Apparently there is no limit to the percentage of explosive

that can be placed in the shell except the mechanical one of having

the walls thick enough to prevent being crushed by the shock of

discharge. In the large projectiles a transverse diaphragm is

introduced to strengthen the walls and to subdivide the charge.

The development of the pneumatic gun has been attended with some other

important discoveries, which may be of interest. It is well known that

mortar fire is very inaccurate, except at fixed long distances, in

consequence of the high angle, the slowness of flight of the

projectile, the variability of the powder pressure, and the inability

to change the elevation and the charge of powder rapidly. In the

pneumatic gun, the complete control of the pressure remedies the most

important of the mortar's defects and makes the fire accurate from

long ranges down to within a few yards of the gun. It is obvious that

the pressure can be usefully controlled in two ways: (1) by keeping

the elevation of the gun fixed and using a valve that can be set to

cut off any quantity of air, according to the range desired; (2) by

keeping the pressure in the reservoir constant, and using a valve

which will cut off the same quantity of air every time, changing the

elevation of the gun according to the distance. Another important

discovery consists in the application of subcalibered projectiles for

obtaining increased range.

The gun is smooth-bored and a full-sized projectile is a cylinder with

hemispherical ends, to the rear of which is attached a shaft having

metal vanes placed at an angle, which causes the projectile to revolve

round its longer axis during flight. A subcalibered projectile,

however, being of less diameter than the bore of the gun, has the

vanes on its exterior, and is held in the axis of the gun by means of

gas checks which drop off as the projectile leaves the muzzle. The

shock to the explosive is, of course, greater than in the full-sized

projectile, but the increase can be calculated, and so far a dangerous

limit has not been reached. From the fifteen-inch gun with a pressure

of 1,000 pounds per square inch and a velocity of about 800 f.s., a

range of 4,000 yards has been obtained at an elevation of 30° 20, with

a ten-inch subcalibered projectile, about eight calibers long and

weighing 500 pounds. This projectile will contain 220 pounds of

blasting gelatine. With improved full-sized projectiles weighing 1,000

pounds, a range of 2,500 yards will doubtless be obtained.

At elevations below 15° these long projectiles are liable to ricochet,

and what is now wanted is a projectile which will stay under water at

all angles of fall and will run parallel to the surface like a

locomotive torpedo. Such a projectile has yet to be invented; but I

have seen a linked shell, which has been experimented with from a

nine-inch powder gun, that partially meets this condition. It is made

of several sections united by means of rope or electric wire in

lengths of 100 to 150 feet. When fired all sections remain together

for some distance; the rear section then first begins to separate;

then the next, and so on. It is primarily intended to envelop an

enemy's vessel, and to remedy the present uncertainty of elevation in

a gun mounted in a pitching boat; but it is found that when it strikes

the water in its lengthened out condition, it will neither dive nor

ricochet, but will continue for some distance just under the surface

until all momentum is lost, when it will sink. This projectile is at

present crude, and has never been tried loaded, but it will probably

be developed into something useful in time.

I have confined my remarks in the foregoing discussion principally to

such methods of using high explosives in shells as have proved

themselves successful beyond an experimental degree, and practically

they reduce themselves to two, viz., using a sluggish explosive in

small quantities from an ordinary powder gun, and using any explosive

from a pneumatic or other mechanical gun. Naturally, the success of

the latter method will soon induce the manufacture of powders having

an abnormally low maximum pressure. There is undoubtedly a field for

the use of such powders in connection with an air space in the gun to

still further regulate the pressure; but nothing of this sort has yet

been attempted. Many methods of padding the shell have been devised

for reducing the shock in powder guns, but the variability of the

powder pressure is too great to have yet rendered any such method

successful. A method was patented by Gruson in Germany of filling a

shell with the two harmless constituents of an explosive and having

them unite and explode by means of a fulminate fuse on striking an

object. He used for the constituents nitric acid and dinitro-benzine,

and was quite successful; but the system has not met with favor, on

account of the inconvenience. The explosive was about four times as

powerful as gunpowder.

That the advantage of using the most powerful explosives is a real one

can be easily shown. The eight inch pneumatic gun in New York harbor,

with a projectile containing fifty pounds of blasting gelatine and

five pounds of dynamite, easily sunk a schooner at 1,864 yards range

from the torpedo effect of the shell falling alongside it.

This same shell, if filled with gunpowder, would have contained but

twenty-five pounds, and have had but one-ninth the power.

The principal European nations are now building armored turrets sunk

in enormous masses of cement, as a result of their experiences with

gun-cotton and melenite. The fifteen inch pneumatic projectile, which

I described as being capable of sinking an armorclad at forty-seven

feet from where it struck, would have been capable of penetrating

fifty feet of cement had it struck upon a fortification. It was not

only a much larger quantity of high explosive than Europeans have

experimented with, but the explosive itself is probably more than

twice as strong as their gun-cotton and five or six times as strong as

their melenite. In the plans of Gen. Brialmont, one of the most

eminent of European engineers, he allows in his fortifications about

ten feet of cement over casements, magazines, etc. It is evident that

this is insufficient for dynamite shells such as I have described.

At Fort Wagner, a sand work built during our war, Gen. Gillmore

estimated that he threw one pound of metal for every 3.27 pounds of

sand removed. He fired over 122,230 pounds of metal, and one night's

work would have repaired the damage. The new fifteen inch pneumatic

shell will contain 600 pounds of blasting gelatine, and judging from

the German experiments at Kummsdorf, which I have cited, one of these

fifteen inch shells would throw out a prodigious quantity of sand;

either 500 pounds to one of shell, or 2,000 pounds to one of shell,

according as the estimate of Gen. Abbot or of Capt. Zalinski is used.

The former considers that the radius of destructive effect increases

as the square root of the charge; the latter that the area of

destructive effect for this kind of work is directly proportional to

the charge.

The effect of the high explosives upon horizontal armor is very great;

but we have yet to learn how to make it shatter vertical armor. No

fact about high explosives is more curious than this, and there is no

theory to account for it satisfactorily. As previously stated, the

French have found that four inches of vertical armor is ample to keep

out the largest melenite shells, and experiments at Annapolis, in

1884, showed that masses of dynamite No. 1, weighing from seventy-five

to 100 pounds, could be detonated with impunity when hung against a

vertical target composed of a dozen one inch iron plates bolted

together.

In conclusion, I may say that in this country we are prone to think

that the perfection of the methods of throwing high explosives in

shell is vastly in favor of an unprotected nation like ourselves,

because we could easily make it very uncomfortable for any vessels

that might attempt to bombard our sea coast cities.

This is true as far as it goes, but unfortunately the use of high

explosives will not stop there. I lately had explained to me the

details of a system which is certainly not impossible for damaging New

York from the sea by means of dynamite balloons. The inventor simply

proposed to take advantage of the sea breeze which blows toward New

York every summer's afternoon and evening. Without ever coming in

sight of land, he could locate his vessel in such a position that his

balloons would float directly over the city and let fall a ton or two

of dynamite by means of a clock work attachment. The inventor had all

the minor details very plausibly worked out, such as locating by means

of pilot balloons the air currents at the proper height for the large

balloons, automatic arrangements for keeping the balloon at the proper

height after it was let go from the vessel, and so on. His scheme is

nothing but the idea of the drifting or current torpedo, which was so

popular during our war, transferred to the upper air. An automatic

flying machine would be one step farther than this inventor's idea,

and would be an exact parallel in the air to the much dreaded

locomotive water torpedo of to-day. There seems to be no limit to the

possibilities of high explosives when intelligently applied to the

warfare of the future, and the advantage will always be on the side of

the nation that is best prepared to use them.

* * * * *

Scientific American Supplement, No. 794, March 21, 1891 · 第 15 / 71 题